{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:CQ325YNIOXJ35DOOOPQEQUSHZP","short_pith_number":"pith:CQ325YNI","schema_version":"1.0","canonical_sha256":"1437aee1a875d3be8dce73e0485247cbcaf42df9000eedc3ac2b76dbe7e6124a","source":{"kind":"arxiv","id":"2411.18434","version":3},"attestation_state":"computed","paper":{"title":"Chiral anomaly and internode scatterings in multifold semimetals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Ipsita Mandal","submitted_at":"2024-11-27T15:17:26Z","abstract_excerpt":"In our quest to unravel the topological properties of nodal points in three-dimensional semimetals, one hallmark property which warrants our attention is the \\textit{chiral anomaly}. In the Brillouin zone (BZ), the sign of the Berry-curvature field's monopole charge is referred to as the chirality ($\\chi$) of the node, leading to the notion of chiral quasiparticles sourcing chiral currents, induced by internode scatterings proportional to the chiral anomaly. Here, we derive the generic form of the chiral conductivity when we have multifold nodes. Since the sum of all the monopole charges in th"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2411.18434","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"cond-mat.mes-hall","submitted_at":"2024-11-27T15:17:26Z","cross_cats_sorted":["hep-th","quant-ph"],"title_canon_sha256":"325a3bb7fe4714d60a22d32f4c2955a131bb3b2e22ecab45a8eaf96fdcaecb1c","abstract_canon_sha256":"2c290e03e225b20162a328a0c10ae85ee752150f43571c753591d7c2116cd14a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:18:40.621270Z","signature_b64":"zMWY9D7sxPilTYAk9IuSCq6CkgqH69mujEiP1nJ0XkbV0P4r/oVUarOmVDChnNwmTaDZZvGoWtdGAyurGUYrAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1437aee1a875d3be8dce73e0485247cbcaf42df9000eedc3ac2b76dbe7e6124a","last_reissued_at":"2026-07-05T11:18:40.620771Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:18:40.620771Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chiral anomaly and internode scatterings in multifold semimetals","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","quant-ph"],"primary_cat":"cond-mat.mes-hall","authors_text":"Ipsita Mandal","submitted_at":"2024-11-27T15:17:26Z","abstract_excerpt":"In our quest to unravel the topological properties of nodal points in three-dimensional semimetals, one hallmark property which warrants our attention is the \\textit{chiral anomaly}. In the Brillouin zone (BZ), the sign of the Berry-curvature field's monopole charge is referred to as the chirality ($\\chi$) of the node, leading to the notion of chiral quasiparticles sourcing chiral currents, induced by internode scatterings proportional to the chiral anomaly. Here, we derive the generic form of the chiral conductivity when we have multifold nodes. Since the sum of all the monopole charges in th"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2411.18434","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2411.18434/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2411.18434","created_at":"2026-07-05T11:18:40.620834+00:00"},{"alias_kind":"arxiv_version","alias_value":"2411.18434v3","created_at":"2026-07-05T11:18:40.620834+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2411.18434","created_at":"2026-07-05T11:18:40.620834+00:00"},{"alias_kind":"pith_short_12","alias_value":"CQ325YNIOXJ3","created_at":"2026-07-05T11:18:40.620834+00:00"},{"alias_kind":"pith_short_16","alias_value":"CQ325YNIOXJ35DOO","created_at":"2026-07-05T11:18:40.620834+00:00"},{"alias_kind":"pith_short_8","alias_value":"CQ325YNI","created_at":"2026-07-05T11:18:40.620834+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.04498","citing_title":"Reflections of topological properties in the planar-Hall response for semimetals carrying pseudospin-1 quantum numbers","ref_index":108,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CQ325YNIOXJ35DOOOPQEQUSHZP","json":"https://pith.science/pith/CQ325YNIOXJ35DOOOPQEQUSHZP.json","graph_json":"https://pith.science/api/pith-number/CQ325YNIOXJ35DOOOPQEQUSHZP/graph.json","events_json":"https://pith.science/api/pith-number/CQ325YNIOXJ35DOOOPQEQUSHZP/events.json","paper":"https://pith.science/paper/CQ325YNI"},"agent_actions":{"view_html":"https://pith.science/pith/CQ325YNIOXJ35DOOOPQEQUSHZP","download_json":"https://pith.science/pith/CQ325YNIOXJ35DOOOPQEQUSHZP.json","view_paper":"https://pith.science/paper/CQ325YNI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2411.18434&json=true","fetch_graph":"https://pith.science/api/pith-number/CQ325YNIOXJ35DOOOPQEQUSHZP/graph.json","fetch_events":"https://pith.science/api/pith-number/CQ325YNIOXJ35DOOOPQEQUSHZP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CQ325YNIOXJ35DOOOPQEQUSHZP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CQ325YNIOXJ35DOOOPQEQUSHZP/action/storage_attestation","attest_author":"https://pith.science/pith/CQ325YNIOXJ35DOOOPQEQUSHZP/action/author_attestation","sign_citation":"https://pith.science/pith/CQ325YNIOXJ35DOOOPQEQUSHZP/action/citation_signature","submit_replication":"https://pith.science/pith/CQ325YNIOXJ35DOOOPQEQUSHZP/action/replication_record"}},"created_at":"2026-07-05T11:18:40.620834+00:00","updated_at":"2026-07-05T11:18:40.620834+00:00"}